In Situ Formation of Zwitterionic Ligands: Changing the Passivation Paradigms of CsPbBr3 Nanocrystals

CsPbBr3 nanocrystals (NCs) passivated by conventional lipophilic capping ligands suffer from colloidal and optical instability under ambient conditions, commonly due to the surface rearrangements induced by the polar solvents used for the NC purification steps. To avoid onerous postsynthetic approaches, ascertained as the only viable stability-improvement strategy, the surface passivation paradigms of as-prepared CsPbBr3 NCs should be revisited. In this work, the addition of an extra halide source (8-bromooctanoic acid) to the typical CsPbBr3 synthesis precursors and surfactants leads to the in situ formation of a zwitterionic ligand already before cesium injection. As a result, CsPbBr3 NCs become insoluble in nonpolar hexane, with which they can be washed and purified, and form stable colloidal solutions in a relatively polar medium (dichloromethane), even when longly exposed to ambient conditions. The improved NC stability stems from the effective bidentate adsorption of the zwitterionic ligand on the perovskite surfaces, as supported by theoretical investigations. Furthermore, the bidentate functionalization of the zwitterionic ligand enables the obtainment of blue-emitting perovskite NCs with high PLQYs by UV-irradiation in dichloromethane, functioning as the photoinduced chlorine source.

S ince the first report in 2015, 1 cesium lead-halide perovskites nanocrystals (CsLHP NCs) are currently at the forefront of research on emissive materials with marked propensities for light-harvesting technologies and optoelectronic applications. 2−4 However, the huge potential of CsLHP NCs is undermined by the ionic nature of the perovskite lattices, which induces highly dynamic bindings between the NC surface and its organic capping ligands. Typically, the passivating agents consist of ionic pairs of an anion (halide or carboxylate) and a cation (cesium or alkylammonium), 5 resulting in a facile ligand cleavage from the NC surface, due to protonation/deprotonation of the carboxylate/alkylammonium couples favored by air and moisture exposure of the colloidal solutions. 6 These processes manifest themselves with the loss of colloidal stability and structural integrity of the perovskite NCs, 7,8 and the conventional purification ap-proaches (based on their precipitation with polar solvents) dramatically amplify the effects of proton transfer processes and remove most of the capping ligands from the NC surface, compromising their structural integrity. 9 Remarkable progress in obtaining stable CsLHP NCs has been reached by strengthening the binding of the capping ligands to the NC surface with robust passivating agents identified in quaternary dimethyldidodecylammonium bromide, 10−13 zwitterionic compounds, 14−18 alkylphosphonic acids, 19,20 bidentate agents, 21,22 and electron-donating ligands. 23−25 Due to their poor availability and/or low solubility in the reaction conditions (particularly evident for ionic species), 26 these capping ligands are often introduced onto the NC surface with onerous postsynthetic approaches. Although leading to an effective improvement of the optical properties and/or stability of the modified NCs, these postpreparative methods can also trigger irreversible structural, morphological, and spectroscopic transformations of the recipient NCs. 27 To overcome these problems, in this work we have developed a straightforward synthetic procedure for passivating CsPbBr 3 NCs through the in situ formation of a zwitterionic ligand via the SN 2 reaction between an additional halide source (8-bromooctanoic acid) and oleylamine used as the surfactant. The formed zwitterionic ligand can adhere to the NC surface through the synergistic interaction with both the dialkylammonium and the carboxylate functionalities. This effective passivation reduces the solubility of the resulting NCs in nonpolar hexane, which can thus be used for the purification stages.
As shown in Figure 1A, along with the conventional PbBr 2 precursor, the proposed synthetic protocol exploited an additional bromide source (8-bromooctanoic acid, BOA), which is endowed with a potential ligand functionality through the carboxylic group, providing "extra" halide anions (Supporting Information for details). The main reaction occurring during the incubation time (before cesium introduction) is schematically depicted in Figure 1B. The OLAm nucleophile can generate bromide ions by the SN 2 reaction involving the only electrophile present in the reaction mixture (BOA, containing a bromine leaving group), yielding a bifunctionalized ligand, which prevalently exists in solution as a zwitterion containing the dialkylammonium and the carboxylate moieties (vide infra), both potentially interacting with the NC surface ( Figure 1B). After the NC isolation following the removal of the supernatant solution from the first centrifugation, the precipitated fluorescent NCs resulted in being insoluble in hexane, allowing us to design a washing protocol without employing aggressive polar solvents (methyl acetate, methanol, or acetone). The purification of NCs was thus carried out by washing them twice with hexane, before the final dispersion in DCM, as described in Figure 1C.
To rationalize this unconventional behavior, we synthesized a batch of CsPbBr 3 NCs under the same reaction conditions except for the use of 1-bromooctane (BO) as the additional bromide source in the substitution of BOA, therefore excluding the formation of the zwitterionic ligand (Scheme S2). 28 As predictable, the obtained fluorescent material directly isolated from the reaction mixture after the centrifugation resulted in being colloidally dispersible in hexane. Therefore, the different behavior exhibited by CsPbBr 3 NCs in terms of colloidal stability/instability in relation to the employed dispersing medium can only be ascribed to the presence of the zwitterionic ligand.
To ascertain the role of the zwitterion in the surface passivation, we investigated the surface chemistry of our bifunctional ligand-modified CsPbBr 3 NCs by nuclear magnetic resonance ( 1 H NMR) analyses. As shown in Figure  2A, the full 1 H NMR spectrum of an aliquot of the reaction mixture produced before cesium injection and dissolved in CDCl 3 was compared to the spectra of the pristine ligands (OLAm and BOA). The comparison evidenced the complete conversion of BOA during the incubation period, as confirmed by the disappearance of the proton signals attributable to its peculiar −CH 2 Br functionality ( Figure 2A; Supporting Information for details). This observation implies the evolution of new organic species (not containing the −CH 2 Br functionality), which simultaneously generate bromide ions in the reaction mixture ( Figures S1 and S2).
The 1 H NMR spectrum of purified CsPbBr 3 NCs clearly evidence a different composition of the organic shell with respect to the pristine ligands ( Figure 2B). The most striking aspect is the absence of other contaminants, including the residual reaction solvent (ODE), and only two washing cycles with hexane are needed to remove all contaminant species weakly bound to the NC surface.
To reveal the nature of the organic species bound to the surface of our NCs and rationalize the peculiar behavior of  Nano Letters pubs.acs.org/NanoLett Letter their organic shell, 29 we inspected the diagnostic 1 H NMR region ascribable to the protons adjacent to the functional groups of the capping ligand ( Figure 2C; Supporting Information for details). In the case of the purified CsPbBr 3 NCs, only two sets of proton signals clearly attributable to the dialkylammonium (ε) and the carboxylate (ϕ) functionalities are observable in the 1 H NMR spectrum, while the ratio between their integrals (ε:ϕ = 2:1) confirms that the bidentate ligand is the only structure composing the organic shell of our NCs. The interaction of the zwitterionic ligand with the NC surface was confirmed by 2D-NOESY investigations, which evidenced the generation of negative cross-peaks associable to proton signals of the bidentate passivating agent ( Figure 2D). The interaction of the zwitterionic ligand with the NC surface  through charged moieties was also ascertained by IR analyses, which showed the presence of a broad band (centered at ∼1540 cm −1 ) ascribable to the carboxylate functionality and absent in the spectra of the pristine ligands ( Figure 2E). We analyzed the elemental composition of the inorganic core of our NCs via scanning electron microscope coupled with energy dispersive X-ray spectroscopy (SEM-EDS). The experimentally observed elemental composition of our NCs (Cs 1.2 Pb 1.0 Br 3.1 ) suggests a slight excess of cesium and bromine with respect to stoichiometry, indicating that a significant contribution to the NC passivation involving the zwitterionic ligand should occur through adsorption onto CsBr-rich surfaces ( Figure 2F).
In order to shed light on the passivation mechanism and binding mode of the zwitterionic ligand, we carried out a DFTbased computational study on the CsBr-terminated (010) perovskite surface (Supporting Information for details). As shown in Figure 3, the bidentate mode (denoted as COO +NH 2 ) is significantly more stable than the corresponding open configuration modes, 30 in which binding occurs through one of the carboxylate oxygens (denoted as COO) or through the dialkylammonium group (denoted as NH 2 ). 12,31,32 This holds true for calculations performed both in vacuum and in solvents of different polarity (hexane or DCM). According to our calculations, monodentate binding with the dialkylammonium group is not stable at high surface coverages (Θ, 0.4 ligand/nm 2 ) and relaxes to the COO+NH 2 bidentate mode configuration. We obtained a strong binding energy (E b = −3.81 eV) for the zwitterionic ligand in the bidentate binding mode (COO+NH 2 ) to this perovskite surface in DCM at low Θ (0.1 ligand/nm 2 ), which explains the remarkable stability of the purified CsPbBr 3 NCs in such medium (vide infra).
Binding energies ( Figure S3) and short binding atom-surface distances ( Figure S4−S5) suggest strong adsorption of the bidentate zwitterionic ligand to the ideal CsPbBr 3 surface, which accounts for the removal of other possible passivating agents during the washing stages of the NCs with hexane.
We ascertained that also the presence of surface point defects favors the bidentate anchoring of the zwitterionic ligand (Def-COO+NH 2 mode in Figure 4 and Figures S6−S7), as this configuration is stable both in DCM (E b = −5.37 eV) and in hexane (E b = −4.44 eV). Furthermore, a different bidentate binding mode, denoted as Def-COO+NH 2 (CH 2 ) in Figure 4, resulted in an efficient passivation of the NC defective surface (E b = −2.31 to −3.23 eV). In such a configuration, the Cs + vacancy is filled by a methylene group of the aliphatic chain, while the dialkylammonium group forms hydrogen bonds with the adjacent bromine atoms.
Conversely, the monodentate binding mode (Def-NH 2 ) is stable only at low surface coverages and evolves to the expected bidentate mode with the dialkylammonium and the carboxylate moieties saturating Cs + and Br − vacancies, respectively, for high surface coverages. It is important to note that in the Def-NH 2 binding mode at low surface coverages, which is remarkably stable in hexane (E b = −5.67 eV), the zwitterionic ligand provides a polar surrounding to the NC surface due to the peripheral carboxylate group, and could be held responsible for the NC insolubility in hexane.
The morphological assessment of the synthesized NCs, performed by transmission electron microscopy (TEM), revealed the formation of nanocubes with average sizes of 21.4 ± 4.1 nm ( Figure S8). The formation of relatively large nanoparticles can be ascribed to the presence of dialkylammonium-based ligands, which do not efficiently compete with Nano Letters pubs.acs.org/NanoLett Letter cesium cations during crystal growth. The optical characterization of purified CsPbBr 3 NCs revealed a sharp excitonic absorption peak at 505 nm and a narrow PL emission band centered at 516 nm (fwhm = 18 nm, Figure 5A). The relatively small Stokes shift suggests that the emission photons exclusively emerge from direct exciton recombination. Analogously to the nanoparticles with a low surface coverage, 33 the emission intensity of our purified CsPbBr 3 NCs measured in diluted DCM solution (PLQY = 89%) is comparable with that of the as-synthesized CsPbBr 3 NCs without the zwitterionic passivating agents (PLQY = 95%, Figure S9). In order to gain insight into the exciton recombination dynamics, we carried out time-resolved PL measurements ( Figure 5B), which have evidenced a single lifetime component (4.0 ns) associated with the high QY value, thus confirming the excellent optical properties of our purified CsPbBr 3 NCs. The compatibility of DCM with the long-term stability of the purified NCs was evaluated by monitoring the PLQY of their stock solution stored in ambient conditions. As shown in Figure 5C, the PLQY of our CsPbBr 3 NCs did not exhibit substantial variations over time (90 days), testifying the robustness of the passivation offered by the zwitterionic ligand. In comparison, the PLQY of as-synthesized conventional CsPbBr 3 NCs stored in DCM was drastically degraded, dropping to values as low as 25% ( Figure S9) during the same time. However, the main drawback concerning the use of DCM as the solvent for dispersing CsLHP NCs resides in the well-documented attitude of dihalomethanes to be photoreduced by perovskite NCs forming halide anions potentially available for halide-exchange processes. 34 Remarkably, under indirect daylight, the emission spectra of CsPbBr 3 NCs and the relevant PLQY remained unchanged over time when dispersed in DCM, indicating that no anion exchange occurs in the solution of NCs in their respective solvents used for their storage.
Since only the interfacial electron transfer from the photoexcited CsLHP NCs can promote the reductive dissociation of dihalomethanes, 35 we exposed our NCs dispersed in DCM to UV-irradiation (365 nm, 8 W/cm 2 ). In this case, we observed the progressive blue shift of their PL maxima upon UV irradiation (λ em = 455 nm after 30 min of irradiation, Figure 5D), while the high PLQY (81%) exhibited by the generated mixed-halide CsLHP NCs at the end of the photoinduced process suggests that surface halide vacancies are not generated during the halide exchange. This result validates the beneficial role of the engineered organic shell in the photostability of our NCs under harsh irradiation conditions. In fact, the same photoinduced halogen exchange carried out on the CsLHP NC passivated by conventional capping ligands 34 caused an analogous blue shift of the emission maxima (λ em = 464 nm upon 30 min of irradiation) accompanied, however, by a remarkable drop of the corresponding PLQY (down to 26% after 30 min of irradiation), as shown in Figures S10−S11.
We also tested our synthetic approach on the preparation of iodine-based NCs by introducing PbI 2 as the halide precursor in the same reaction conditions utilized in this work. For the obtained CsPbBr x I 3−x NCs, we verified a similar behavior with respect to that observed for CsPbBr 3 NCs (Figures S12−S14).
In conclusion, the suitable engineering of the organic shell composition of CsPbBr 3 NCs can reduce their affinity toward apolar solvents (nonaggressive toward the ionic structure of perovskites) allowing the use of hexane for the purification stages in alternative to conventional polar solvents. The CsPbBr 3 NCs prepared following our protocol can be deprived of the organic contaminants without de facto compromise of their optical properties during the purification stages. The purified NCs are dispersible in DCM, in which they are found to be colloidally and optically stable for three months. Highly efficient blue-emitting NCs are obtained by UV-irradiation of the purified CsPbBr 3 NCs passivated by the bidentate capping ligand in DCM as the solvent providing the chloride source for the photoinduced halide exchange.